Suppressed Ion-Scale Turbulence and Critical Density Gradient in the C-2 Field-Reversed Configuration L. Schmitz (UCLA, TAE) with C. Lau, D. Fulton, I. Holod, Z. Lin, (UCI), T. Tajima, M. Binderbauer, H. Gota, B. Deng, J. Douglass (TAE) and the TAE Team Norman Rostoker Memorial Symposium August 24-25, 2015 Irvine, CA 5 0 -5 f D (MHz) 0 1 2 Time (ms)
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Suppressed Ion-Scale Turbulence and Critical Density Gradient in the C-2
Field-Reversed Configuration L. Schmitz (UCLA, TAE)
with C. Lau, D. Fulton, I. Holod, Z. Lin, (UCI), !
T. Tajima, M. Binderbauer, H. Gota, B. Deng, J. Douglass (TAE) and the TAE Team!
!
!!
Norman Rostoker !Memorial Symposium!August 24-25, 2015!
Irvine, CA!!
5
0
-5
f D (
MH
z)
0 1 2Time (ms)
2 L. Schmitz Norman Rostoker
Memorial Symposium
Goal of FRC Turbulence/Transport Studies:�Active Profile, Boundary, and Transport Control
Transport Models,
Dimensionless Scaling
Predictive Kinetic
Turbulence Modeling
Advanced Turbulence/
Profile Measurements
Active Profile,
Boundary, Transport Control
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Memorial Symposium
Outline § Introduction
§ Experimental fluctuation/turbulence studies in the C-2 FRC
§ Gyrokinetic Modeling: FRC core and boundary fluctuations
§ Critical gradients, core/SOL transition and barrier effects
§ Summary
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Memorial Symposium
FRC Geometry / C-2 Parameters
Solenoid coil (External B-Field)
B-Field Null (R)
Separatrix (Rs) Scrape-off layer
Core Plasma
Bez
Typical C-2 Parameters
FRC Core SOL Density (1019 m-‐3)
2-‐4 0.5-‐2
Ti (eV) 600-‐1000 ≤250 Te (eV) ≤ 150 30-‐80 Be (Gauss) ≤ 1200 Sep. Radius (cm)
35-‐45
Neutral Beam Power
≤ 4 MW
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Memorial Symposium
FRC Radial and Parallel Transport� Scrape-off layer (SOL):
Radial and parallel Transport (along z)
τ⊥−1 = 1
r∂∂r
rDr1n∂n∂r
⎛⎝⎜
⎞⎠⎟
Radial transport:
τ−1 = (τii lnRM )
−1
τ−1 = (τii lnRM )
−1
Radial Gradient scale length : If depends on , parallel and perpendicular transport are coupled
-10 -5 0 5 10
0.6
0.4
0.2
z (m)
r (
m)
From continuity (particle conservation:) ∇(nv i ) = −∇⊥ (nv i ) τ = τ⊥
Ln⊥
Ln⊥ = D⊥τ ii lnRM
D⊥
D⊥
Separatrix
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Schematic and Principle of Doppler Backscattering Diagnostic (DBS)
ts=ti-kevExBks=ki-ke
b
c
ke
kIkS
tI,kI
ee .Be,ez
ñ/n: local density fluctuation level ñ(r)/n(r) vs. kθ - here kθ~ 0.5-12 cm-1 (kθρs~1-40)
ExB velocity from Doppler shift of back-scattered signal: ωDoppler = vturb kθ ~ vExBkθ
è vExB ~ ωDoppler / 2ki
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Radial Density Profile and DBS Probing Radii
§ DBS: 6 remote-tunable channels (co-linear beams), probing the FRC core (outside field null) and the SOL
§ Beam path calculated via GENRAY ray/beam tracing, based on reconstructed (CO2) density profiles
ts=ti-kevExBks=ki-ke
b
c
ke
kIkS
tI,kI
ee .Be,ez
60
40
20
0
-20
-40
-60
-60 -40 -20 0 20 40 60
x (cm)
y (c
m)
750+s
MW Launch
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Memorial Symposium
Density Fluctuations Peak Outside Separatrix Very Low Fluctuations in FRC Core
n Fluctuation levels peak outside the separatrix n Very low fluctuation levels in the FRC core
§ Experimental fluctuation/turbulence studies in the C-2 FRC
§ Gyrokinetic Modeling: FRC core and boundary fluctuations
§ Critical gradients, core/SOL transition and barrier effects
§ Summary
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Memorial Symposium
GTC (Gyrokinetic Toroidal Code) Simulations
First-principles, integrated microturbulence simulations; adapted for FRC geometry (Boozer coordinates): Useful for predictive modeling and reduced transport models Input: Experimental (measured) or calculated FRC equilibria Gyrokinetic or kinetic ions, kinetic electrons Local/global simulations, electromagnetic effects Fokker-Planck-collisions Presented here: Results from linear, electrostatic flux-tube simulations, separate calculations for the FRC core and SOL Future work: Coupled SOL/core, kinetic ions, nonlinear runs
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Simulation Geometry, Parameters
Core and SOL local simulation: Realistic C-2 Equilibrium Periodic boundary conditions in z and θ Gyrokinetic ions (D) and electrons, νe,i*=ν/νtransit <<1
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FRC-Core: Ion Modes Suppressed via FLR Effects, only Electron Modes Unstable
Calculated Linear Growth Rate from GTC
Measured Saturated Spectrum
• Spectrum extends to kθρe > 0.3: matches linearly unstable k-range Dominant electron modes; ion modes weak/absent due to FLR* effects:
*Rosenbluth, Krall and Rostoker, NF Suppl. pt1, 143 (1962)
kѡ��ѩe
0.8
0.4
�������
aR/c
s 0.24 0.28 �������
d=1
Core
R/LTe=5.25
no collisions
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Ballooning Structure with/without Collisions
collisionless (ballooning) with collisions (ballooning, virtually no change in mode structure) θ
ζ
ζ
ζ
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Local Gyrokinetic SOL Simulations
i-‐i e-‐i e-‐e 0.0058 0.172 0.082
𝜈*
Gyrokinetic D Ions Drift-kinetic electrons Ti = 5Te, Zeff =1.5 Fokker-Planck Collisions Flux-tube, local �simulation at r/Rs=1.2; periodic boundary in z
⇒ 𝜈*e-‐e=𝜈e-‐e/(vth-‐e/L) (moderate electron collisionality )
SOL
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SOL: Exponential Wavenumber Spectrum;Unstable Ion Modes
#29587-29610, #29750-29802
ρs=[(kTe+kTi)/mi]1/2/ωci
Measured Saturated Spectrum Calculated Linear Growth Rate from GTC (w/collisions)
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Driving Gradients Differ in FRC Core and SOL aR
/cs
3.0
2.0
1.0
00.75 0.8 0.85 0.9 0.95 1.0
de
Core di=1
R/LTi=R/Ln= 6
no collisions
kѡ� ѩe=0.3
∇Te ∇n
No instability below ηe <0.75
Electron drift/Interchange Core modes driven by and curvature
Instability to 1/ηi =0
Density gradient-driven SOL ion drift modes
aR/c
s
0.3
0.2
0.1
00 0.2 0.4 0.6 0.8 1.0
� di
R/LTe= R/LTi
= 6
SOL�de=1
kels= 0.85
w/collisions
SOL Modes are Driven by Core Modes are Driven by
∇Te
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Memorial Symposium
Outline § Introduction
§ Experimental fluctuation/turbulence studies in the C-2 FRC
§ Gyrokinetic Modeling: FRC core and boundary fluctuations
§ Critical gradients, core/SOL transition and barrier effects
§ Summary
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Memorial Symposium
E×B Shear Increases the SOL Critical Gradient
§ Radial density gradient increases after ~0.5 ms (SOL is depleted) § SOL fluctuation increase once critical density gradient is exceeded § Fluctuation decrease once ExB shearing rate increases exceeds the turbulence decorrelation rate: ωΕ×Β>ΔωD (Biglari, Diamond, Terry, Phys. Fluids B1,1989) § The radial correlation length decreases with increasing ExB shear
Density profile time history
6
4
2
0
R/L n
0.14
0.07
0
0 0.5 1.0 1.5 2.0 2.5
1.0
0.5
0
-0.5
Time (ms)
t E�B
, tD (
106 ra
d/s)
ñ/n (a
u)1.5
1.0
0.5
0
h r (c
m)
R/Ln crit
0.6
0.4
0.2
0
0.2
0.4
0.6
r (m
)
2.3
1.9
1.5
1.1
0.7
0.4
0
ne (1019 m-3)
r/Rs=1.1
r/Rs=1.1
r/Rs=0.9
r/Rs=0.9
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Measured Critical Gradient and Calculated Core Linear Threshold from GTC
a R/
c s
2.0
1.5
1.0
0.5
0
R/LTe, R/Ln4.8 5.2 5.6
r/Rs=0.97 Corekele = 0.27kele = 0.30
de= di= 1
2 3 4R/Ln
0.16
0.08
0
ñ/n
(au)
r/Rs ~ 1.15r/Rs = 0.95r/Rs ~ 0.85
kele ~ 0.07-0.28
R/Ln critR/Ln crit
(SOL)(Core)
Measured R/ Ln crit (FRC core/SOL)
FRC core growth rate vs. R/LTe from linear GTC simulation
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2 3 4R/Ln
0.16
0.08
0
ñ/n
(au)
r/Rs ~ 1.15r/Rs = 0.95r/Rs ~ 0.85
kele ~ 0.07-0.28
R/Ln critR/Ln crit
(SOL)(Core)
R/Ln
kels = 0.85kels = 1.70
3 4 5 6
0.4
0.3
0.2
0.1
0a R
/cs
R/Ln
r/Rs=1.2 SOL
kels = 0.85kels = 1.70
3 4 5 6
Measured SOL Critical Density Gradient Similar to Predicted Linear Instability Threshold
Measured R/ Ln crit (FRC core/SOL)
FRC core growth rate vs. R/Ln from linear GTC simulation
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Memorial Symposium
Core-SOL Coupling: Evidence �for Radial Transport Barrier
§ Radial turbulence correlation
length λr ≤ ρi § No evidence of sustained extended radial structures or streamers λr reduced just outside Rs: Evidence of radial transport barrier. § Shear decorrelation just outside the separatrix: ωΕ×Β>ΔωD (Biglari, Diamond, Terry,
Phys. Fluids B1,1989)
-10 0 10
tE
xB, 6
tD
(1
05 r
ad/s
)
r-Rs (cm)
6
4
2
0
>
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Memorial Symposium
Summary • C-2 FRC core: Ion modes stable due to FLR effect; only
electron modes unstable (driven by electron temperature gradient and curvature)
• Moderate, larger-scale ion-mode SOL turbulence observed/predicted; driven by the radial density gradient.
• Strong evidence of radial transport barrier in the SOL. No experimental evidence of sustained large-scale radial structures/streamers (radial correlation length λr < ρi)
• Observed critical SOL density gradient compares well
with predicted linear instability threshold; compatible with required reactor SOL width